Guinier law (interpretation w/o a model)
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Transcript of Guinier law (interpretation w/o a model)
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Guinier law (interpretation w/o a model)
Regardless of particle shape, at small q :
I(q) = (v)2 exp (-qRg)2/3
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Guinier law (interpretation w/o a model)
Regardless of particle shape, at small q :
I(q) = (v)2 exp (-qRg)2/3
ln (q) = ln (v)2 - (Rg2/3) q2
![Page 3: Guinier law (interpretation w/o a model)](https://reader035.fdocuments.us/reader035/viewer/2022070405/56813d05550346895da6aa6e/html5/thumbnails/3.jpg)
Guinier law (interpretation w/o a model)
Regardless of particle shape, at small q :
I(q) = (v)2 exp (-qRg)2/3
ln (q) = ln (v)2 - (Rg2/3) q2
![Page 4: Guinier law (interpretation w/o a model)](https://reader035.fdocuments.us/reader035/viewer/2022070405/56813d05550346895da6aa6e/html5/thumbnails/4.jpg)
Guinier law (interpretation w/o a model)
Regardless of particle shape, at small q :
I(q) = (v)2 exp (-qRg)2/3
ln (q) = ln (v)2 - (Rg2/3) q2
Only holds if:
a. q < 1/Rg
b. dilute
c. Isotropic
d. matrix or solvent scattering is removed
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Guinier law (outline of derivation)(r) is scattering length distribution
A(q) = ∫(r) exp (-iqr) dr
Expand as a power series:
A(q) = ∫(r) dr - i∫qr (r) dr - (1/2!)∫(qr)2 (r) dr + …
Origin at center of mass
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(r) is scattering length distribution
A(q) = ∫(r) exp (-iqr) dr
Expand as a power series:
A(q) = ∫(r) dr - i∫qr (r) dr - (1/2!)∫(qr)2 (r) dr + …
Origin at center of mass
(qr)2 = (qxx + qyy + qzz)2
xy = (1/ v)∫xy (r) dr , etc……
Guinier law (outline of derivation)
0v
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q << v; average intensity/particle, for large # randomly oriented particles:
I(q) = (v)2(1- ((qxx)2 + (qyy)2 + (qzz)2 + 2qxqyxy)
Isotropic:
average x2 = average y2 = average z2 = Rg2/3
average xy = average yz = average zx = 0
I(q) = (v)2(1- ((q Rg)2 /3+ …)
I(q) = (v)2 exp (-qRg)2/3
Guinier law (outline of derivation)
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For non-identical particles, Guinier law gives an average R & average v
Guinier law (outline of derivation)
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Model structures - effect of dense packing
For N spherical particles, radius R, scattering length density
A(q) = A1(q)-iqrj)
Rj = location of center of jth sphere, A1(q) = form factor for single sphere
j=1
N
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Model structures - effect of dense packing
For N spherical particles, radius R, scattering length density
A(q) = A1(q)-iqrj)
Rj = location of center of jth sphere, A1(q) = form factor for single sphere
I(q) = I1(q)-iqrjk)
I(q) = I1(q)(N + -iqrjk))
j=1
N
k=1
N
j=1
N
j=1
N
k≠1
N
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Model structures - effect of dense packing
For N spherical particles, radius R, scattering length density
A(q) = A1(q)-iqrj)
Rj = location of center of jth sphere, A1(q) = form factor for single sphere
I(q) = I1(q)-iqrjk)
I(q) = I1(q)(N + -iqrjk))
j=1
N
k=1
N
j=1
N
j=1
N
k≠1
N
independent scattering from particles
correlated scattering betwn particles
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Model structures - effect of dense packing
For N spherical particles, radius R, scattering length density
A(q) = A1(q)-iqrj)
Rj = location of center of jth sphere, A1(q) = form factor for single sphere
I(q) = I1(q)-iqrjk)
I(q) = I1(q)(N + -iqrjk))
<n> g(r) dr = probability of finding another particle in dr at distance r
from a given particle (<n> = average # density of particles)
I(q) = N I1(q)(1 + <n> ∫g(r)-iqr)dr)
Or:
I(q) = N I1(q)(1 + <n>∫(g(r) - 1)-iqr)dr)
j=1
N
k=1
N
j=1
N
j=1
N
k≠1
N
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Model structures - effect of dense packing
<n> g(r) dr = probability of finding another particle in dr at distance r
from a given particle (<n> = average # density of particles)
I(q) = N I1(q)(1 + <n> ∫g(r)-iqr)dr)
Or:
I(q) = N I1(q)(1 + <n>∫(g(r) - 1)-iqr)dr)
Isotropic:
I(q) = N I1(q)(1 + <n>∫4r2(g(r) - 1)sin (qr))/(qr) dr)
One result:
as fraction of volume occupied by spheres <n>v
0
∞
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Model structures - effect of dense packing
One result:
as fraction of volume occupied by spheres <n>v ,low q intensity is suppressed.
q
I(q)/N (v)2
hi <n>v
lo <n>v
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Model structures - effect of dense packing
Anisotropic particles give similar result, altho more complicated.